{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:YFTM5EJZCONBXB4HJBMAU3L6XT","short_pith_number":"pith:YFTM5EJZ","canonical_record":{"source":{"id":"1411.3916","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-14T14:21:18Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a35a2e7e345cefd4ab300ee6e95c656fd4de3e88455f2282cec7816eb0597da2","abstract_canon_sha256":"bb6c8e57f3eef9baf49c5042be415e1bdb1edb5adc1d4d75d281a909845be0b4"},"schema_version":"1.0"},"canonical_sha256":"c166ce9139139a1b878748580a6d7ebcfb760a60b5a6594b532bb159a1a9a6c6","source":{"kind":"arxiv","id":"1411.3916","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.3916","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"arxiv_version","alias_value":"1411.3916v1","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.3916","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"pith_short_12","alias_value":"YFTM5EJZCONB","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YFTM5EJZCONBXB4H","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YFTM5EJZ","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:YFTM5EJZCONBXB4HJBMAU3L6XT","target":"record","payload":{"canonical_record":{"source":{"id":"1411.3916","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-14T14:21:18Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a35a2e7e345cefd4ab300ee6e95c656fd4de3e88455f2282cec7816eb0597da2","abstract_canon_sha256":"bb6c8e57f3eef9baf49c5042be415e1bdb1edb5adc1d4d75d281a909845be0b4"},"schema_version":"1.0"},"canonical_sha256":"c166ce9139139a1b878748580a6d7ebcfb760a60b5a6594b532bb159a1a9a6c6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:37.369867Z","signature_b64":"vwFFv+gsBzXbAbd8yyii+2F7VMGgjtMaL/D7CgD559n7INC8ISRAeBqZ1jnkAb3fqifZ0xxLp2s5ND3c6milCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c166ce9139139a1b878748580a6d7ebcfb760a60b5a6594b532bb159a1a9a6c6","last_reissued_at":"2026-05-18T02:37:37.369458Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:37.369458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.3916","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:37:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CMCAjIPt8h8iwAW3tvsxX+ZrvjFbiOZxHg2eq2b7iikBACERWDiPa8XJQp25MuPz4bKjRwWMmTFkDFUZPzhvCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:38:12.708077Z"},"content_sha256":"4b609271bdf2572b8042e2549cb73453674038c72c1a9a22f658b67f00f85158","schema_version":"1.0","event_id":"sha256:4b609271bdf2572b8042e2549cb73453674038c72c1a9a22f658b67f00f85158"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:YFTM5EJZCONBXB4HJBMAU3L6XT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Form factors for $\\mathrm B_\\mathrm s \\to \\mathrm K \\ell \\nu$ decays in Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Alberto Ramos, Anosh Joseph, Fabio Bernardoni, Felix Bahr, Hubert Simma, John Bulava, Rainer Sommer","submitted_at":"2014-11-14T14:21:18Z","abstract_excerpt":"We present the current status of the computation of the form factor $f_+ (q^2)$ for the semi-leptonic decay $\\mathrm B_\\mathrm s \\to \\mathrm K \\ell \\nu$ by the ALPHA collaboration. We use gauge configurations which were generated as part of the Coordinated Lattice Simulations (CLS) effort. They have $N_\\mathrm f=2$ non-perturbatively $O(a)$ improved Wilson fermions, and pion masses down to $\\approx 250 \\,\\mathrm {MeV}$ with $m_\\pi L \\geq 4$. The heavy quark is treated in non-perturbative Heavy Quark Effective Theory (HQET).\n  We discuss how to extract the form factors from the correlation func"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.3916","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:37:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oC/x9wy3e+/o4z+U4BDak5eL/lCZQxndLR5d5xVq8le7A8jgToCDYpq1Lw/zsOA0H4Mpr49dD/x/+Z8jIQ8GCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:38:12.708476Z"},"content_sha256":"75ae052c3b22deaefcd88f39eb6a607aaaf5e6d74bac4557c1846b66105b3676","schema_version":"1.0","event_id":"sha256:75ae052c3b22deaefcd88f39eb6a607aaaf5e6d74bac4557c1846b66105b3676"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/bundle.json","state_url":"https://pith.science/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T07:38:12Z","links":{"resolver":"https://pith.science/pith/YFTM5EJZCONBXB4HJBMAU3L6XT","bundle":"https://pith.science/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/bundle.json","state":"https://pith.science/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YFTM5EJZCONBXB4HJBMAU3L6XT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:YFTM5EJZCONBXB4HJBMAU3L6XT","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"bb6c8e57f3eef9baf49c5042be415e1bdb1edb5adc1d4d75d281a909845be0b4","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-14T14:21:18Z","title_canon_sha256":"a35a2e7e345cefd4ab300ee6e95c656fd4de3e88455f2282cec7816eb0597da2"},"schema_version":"1.0","source":{"id":"1411.3916","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.3916","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"arxiv_version","alias_value":"1411.3916v1","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.3916","created_at":"2026-05-18T02:37:37Z"},{"alias_kind":"pith_short_12","alias_value":"YFTM5EJZCONB","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YFTM5EJZCONBXB4H","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YFTM5EJZ","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:75ae052c3b22deaefcd88f39eb6a607aaaf5e6d74bac4557c1846b66105b3676","target":"graph","created_at":"2026-05-18T02:37:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We present the current status of the computation of the form factor $f_+ (q^2)$ for the semi-leptonic decay $\\mathrm B_\\mathrm s \\to \\mathrm K \\ell \\nu$ by the ALPHA collaboration. We use gauge configurations which were generated as part of the Coordinated Lattice Simulations (CLS) effort. They have $N_\\mathrm f=2$ non-perturbatively $O(a)$ improved Wilson fermions, and pion masses down to $\\approx 250 \\,\\mathrm {MeV}$ with $m_\\pi L \\geq 4$. The heavy quark is treated in non-perturbative Heavy Quark Effective Theory (HQET).\n  We discuss how to extract the form factors from the correlation func","authors_text":"Alberto Ramos, Anosh Joseph, Fabio Bernardoni, Felix Bahr, Hubert Simma, John Bulava, Rainer Sommer","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-14T14:21:18Z","title":"Form factors for $\\mathrm B_\\mathrm s \\to \\mathrm K \\ell \\nu$ decays in Lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.3916","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:4b609271bdf2572b8042e2549cb73453674038c72c1a9a22f658b67f00f85158","target":"record","created_at":"2026-05-18T02:37:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"bb6c8e57f3eef9baf49c5042be415e1bdb1edb5adc1d4d75d281a909845be0b4","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-14T14:21:18Z","title_canon_sha256":"a35a2e7e345cefd4ab300ee6e95c656fd4de3e88455f2282cec7816eb0597da2"},"schema_version":"1.0","source":{"id":"1411.3916","kind":"arxiv","version":1}},"canonical_sha256":"c166ce9139139a1b878748580a6d7ebcfb760a60b5a6594b532bb159a1a9a6c6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c166ce9139139a1b878748580a6d7ebcfb760a60b5a6594b532bb159a1a9a6c6","first_computed_at":"2026-05-18T02:37:37.369458Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:37:37.369458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vwFFv+gsBzXbAbd8yyii+2F7VMGgjtMaL/D7CgD559n7INC8ISRAeBqZ1jnkAb3fqifZ0xxLp2s5ND3c6milCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:37:37.369867Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.3916","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b609271bdf2572b8042e2549cb73453674038c72c1a9a22f658b67f00f85158","sha256:75ae052c3b22deaefcd88f39eb6a607aaaf5e6d74bac4557c1846b66105b3676"],"state_sha256":"9818e9042734315534bbe42a0b7fce4f808596a6d8b0d3b3cd88c53df9b3481e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OwizmbRRhy3NPuuEp86tb3sAh4gdldv0afCPYJTm8TEt0+L1XnoMjVcqK6jvGVB1DAPvz4tG57hAivLq63N2AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T07:38:12.711601Z","bundle_sha256":"50d49b90d6d30d5eccb8382ca64e0489119d58dd90e043b98610edef2ac8b578"}}